Upload
others
View
4
Download
0
Embed Size (px)
Citation preview
1189
Towards open-ended evolution in self-replicatingmolecular systemsHerman Duim1 and Sijbren Otto*2
Review Open Access
Address:1Zernike Institute for Advanced Materials, University of Groningen,Nijenborgh 4, 9747 AG Groningen, The Netherlands and 2StratinghInstitute for Chemistry, University of Groningen, Nijenborgh 4, 9747AG Groningen, The Netherlands
Email:Sijbren Otto* - [email protected]
* Corresponding author
Keywords:autocatalysis; open-ended evolution; origin of life; self-replication;synthetic life
Beilstein J. Org. Chem. 2017, 13, 1189–1203.doi:10.3762/bjoc.13.118
Received: 06 December 2016Accepted: 18 May 2017Published: 21 June 2017
This article is part of the Thematic Series "From prebiotic chemistry tomolecular evolution".
Guest Editor: L. Cronin
© 2017 Duim and Otto; licensee Beilstein-Institut.License and terms: see end of document.
AbstractIn this review we discuss systems of self-replicating molecules in the context of the origin of life and the synthesis of de novo life.
One of the important aspects of life is the ability to reproduce and evolve continuously. In this review we consider some of the
prerequisites for obtaining unbounded evolution of self-replicating molecules and describe some recent advances in this field.
While evolution experiments involving self-replicating molecules have shown promising results, true open-ended evolution has not
been realized so far. A full understanding of the requirements for open-ended evolution would provide a better understanding of
how life could have emerged from molecular building blocks and what is needed to create a minimal form of life in the laboratory.
1189
IntroductionMankind has always pondered upon its own existence and has
sought to understand the origin of life. This led us to trace back
our roots, from the great apes to a last universal common
ancestor, a simple cellular lifeform from which all other
present-day organisms have descended. Ultimately this leads us
to one of the great questions in science; how can life emerge
from inanimate matter? And even more interestingly, can we
achieve such a process in the lab and create life from scratch?
There are many different theories surrounding the origin of life
and several attempts have been made to realize the synthesis of
de novo life. All theories involve the presence of molecules that
can create copies of themselves at some stage. It remains
unclear whether such molecules were already important at the
very early stages of the origin of life or whether life started with
large autocatalytic networks [1] and specific molecules that
store genetic information only appeared later. These self-repli-
cating molecules carry hereditary information in the form of
their molecular structure that can be passed on to successive
generations. If mutations occur during the replication process,
genetic information can change from one generation to the next.
Natural selection can act on these variations, favoring those
Beilstein J. Org. Chem. 2017, 13, 1189–1203.
1190
varieties that are beneficial for the stability and reproduction of
the replicator. Under the right conditions, such Darwinian type
evolution can eventually lead to diversification and complexifi-
cation of the molecules in the system.
This review aims to provide an insight into the historical back-
ground and recent developments in the field of in vitro evolu-
tion of self-replicating molecules. To do so, we will first cover a
few important principles of Darwinian evolution and will show
how these concepts apply to the case of molecular self-replica-
tion. This is followed by a description of some self-replicating
systems and their properties, starting from the very first report
on self-replication to more elaborate systems. Finally, some
recent experiments concerning in vitro evolution of self-repli-
cating molecules and networks will be discussed. We argue
that, although systems that show intriguing evolutionary capa-
bilities have been devised, there is still a long way to go before
a system that is capable of true undirected or open-ended evolu-
tion has been realized. Worryingly, the phenomenon of open-
ended evolution in itself is currently not well-defined nor under-
stood. If we are to create life in the lab, a thorough knowledge
of this concept and its prerequisites is probably essential.
Review1 Requirements for Darwinian evolutionOne of the most remarkable and key features of life is the fact
that it has a strong tendency (or, at least ability) to diversify and
increase in complexity. Whereas life once must have started out
as a comparatively simple and primitive form, it has diversified
into a vast variety of species ranging from aquatic to airborne
ones. The principles governing this diversification in biological
systems were already described by Darwin in his famous work
On the Origin of Species, but are still not understood in full
detail [2]. It was only in the 1960’s that Spiegelman extended
the scope of Darwinian evolution to chemical systems by
studying the evolution of RNA-complexes [3]. In these experi-
ments RNA was replicated using enzymes “borrowed” from
contemporary biology. The outcome of the selection experi-
ments was the shortening of the RNA sequence, as shorter se-
quences could be replicated faster. It was soon realized that a
better understanding about how evolution acts on the molecular
level would not only provide valuable insights into the origin of
life and the emergence of species, but it could also pave the way
towards the realization of synthetic life.
In biology, Darwinian evolution in a chemical system can be
considered to be the result of an interplay of the three different
processes that are summarized in Figure 1 [4]. These concepts
can, in principle, be extended to what we will consider as
Darwinian evolution in chemical systems. First the parent mole-
cule, or replicator, is replicated to yield a large number of
copies. This can for instance be achieved via an autocatalytic
cycle, as will be discussed below. Mutation involves the emer-
gence of a difference between the parent template and its
copies. The accuracy of the replication process of DNA is gen-
erally safeguarded by sophisticated enzymes, but systems that
lack such machinery are more prone to occasional errors during
replication. Mutations, however, might actually be advanta-
geous for the replicator if the newly formed copies are more
stable, replicate more efficiently or prevail under a change of
environment. If such advantageous mutations arise, competi-
tion between different replicators might occur, leading to a
process of natural selection and survival of the fittest replicator.
We consider replication, mutation and selection to be necessary
and sufficient conditions for Darwinian evolution.
Figure 1: Three processes involved in Darwinian evolution. Speciesmust be replicated to obtain a large population. During the replicationprocess mutations can occur, on which natural or artificial selectioncan then take place.
1.1 ReplicationDuring replication a large number of copies of the replicator is
produced via an autocatalytic process. In animals or other life-
forms it is quite clear that reproduction leads to a transfer of
genetic information from the parent to the offspring. Not only
are the vital structures of the organism transferred but also some
peculiarities like a specific eye color or a hereditary disease is
passed on to the next generation. The transfer of information in
replicating molecules may be less obvious, but if one considers
a polymer with a specific sequence of subunits, it is clear that
some form of genetic information is transferred if the copies
have an identical sequence to the parent molecule.
The survival of a particular molecular structure under a set of
environmental conditions depends on both the rate of replica-
tion and the rate of decomposition of this replicator. If a repli-
cator decomposes at a higher rate than that it is produced, that
particular replicator may become extinct. If, on the other hand,
Beilstein J. Org. Chem. 2017, 13, 1189–1203.
1191
the sequence and structure of the molecule is such that the repli-
cation rate exceeds its destruction rate, the replicator is suffi-
ciently adapted to its environment and will persist under the
given conditions.
1.2 MutationThe environmental conditions, to which a set of replicators is
exposed however, may not be in a steady-state. Instead, the
environment may be continuously changing. Consider for
instance changes in temperature, acidity, light intensity and
humidity to which a system will inevitably be subjected. A
replicator that is very well adapted to a certain environment,
might not persist at a later time when the environmental condi-
tions have changed. In fact, if it were not for the presence of
small mutations in the genetic information, a species would be
very fragile. If the number of mutations is only small compared
to the length of the molecule, hereditary information is still
largely preserved. Moreover, the mutants may be better adapted
to the new environmental conditions than their predecessors. If
the mutants indeed have a higher rate of accumulation than their
parents, they will eventually overtake their parents and will
become the new dominant species. In practice a replicator gen-
erally has to exhibit exponential growth in order to dominate
over a weaker replicator [5-7].
Eigen et al. noted, however, that the case is somewhat more
complicated than a single type of mutant replicator overtaking
another replicator. They introduced the concept of quasi-
species, as an analogue to conventional species in biology [8].
A quasi-species consists of a master sequence with a dynamic
distribution of closely related mutants. This concept captures
the fact that for relatively high mutation rates not a single fittest
replicator, but rather a distribution of closely related mutants
survives. The mutants in this distribution around a master se-
quence all replicate at a different rate and are cross-catalytic,
which leads to the production of further mutants. Selection in
these systems thus does not act on the level of individual
mutants, but rather on the entire quasi-species [8-10]. Such
quasi-species behavior was recently reported in an in vitro
evolution experiment with replicating RNA species [11].
There is of course a constraint on the number of mutations that
can occur without losing too much hereditary information from
the parent molecules. In the same work, Eigen showed that
unless mutation rates were significantly diminished, the
increase in the length of the genome would unavoidably lead to
a catastrophic loss of hereditary information. That is, the repli-
cation process of a long molecule requires a much higher
fidelity than that of a smaller molecule. If the rate at which
errors in the replication occur exceeds a certain error threshold,
the genetic information will disintegrate and the species will go
extinct [8,12]. In fact, the reason that viruses are so good in
adapting to different environments and always seem to be one
step ahead of the defense mechanisms of the host is because the
replication process of the viral genome operates very close to
the error threshold, allowing for as many mutations as possible
without the loss of genetic information [12,13].
1.3 SelectionIn biology natural selection operates on the phenotype, i.e., the
observable traits of a species. An individual that is better
adapted to its environment is more likely to survive then one
that is less adapted. This higher survival rate will lead to a
larger amount of offspring for that type of individual, favoring
their presence in the population. The phenomenon of natural
selection can also operate at the molecular level. This requires
experiments to be run under conditions where replication and
replicator destruction occur in parallel. Such conditions were
employed in only a small subset of the work on self-replicating
molecules where the emphasis has mostly been on replication in
the absence of destruction. Which replicators then end up being
selected depends on their rates of replication relative to their
rate of destruction, or, as proposed by Pross, their dynamic
kinetic stability [14]. Selection in the Darwinian sense requires
extinction of the weaker replicators, so that only the fitter ones
remain. There are some detailed kinetic considerations that lead
to specific mechanistic requirements for the replication process.
Szathmary and Lifson showed that in a scenario where differ-
ent replicators compete for common building blocks, extinction
of the weakest replicators occurs only if the kinetic order of the
replicator in the replication process is at least equal to the order
of the replicator in the destruction process [5,6]. As for most
plausible mechanisms the destruction process is first order in
replicator, this implies that the replication process must also be
at the least first order in replicator; i.e., replicators need to be
able to grow exponentially in order to exhibit Darwinian evolu-
tion in the most common scenarios. This consideration has
spurred many efforts to develop exponential replicators, which
are far from trivial to produce (vide infra). But even with expo-
nential replicators, Darwinian evolution does not necessarily
lead to complexification and the spontaneous emergence of new
function, as the Spiegelman experiments made painfully clear
[3].
Yet, in order to obtain a form of life from a molecular system, it
must be able to grow increasingly complex and diverse.
Systems that undergo such undirected diversification may in the
end give rise to ecosystems full of complex organisms or struc-
tures [15]. Note that these organisms then would all be part of
an evolving ecosystem, and it has been argued that a proper and
complete description of life should therefore not only be at the
individual level but also at the level of entire ecosystems [16].
Beilstein J. Org. Chem. 2017, 13, 1189–1203.
1192
1.4 Dynamic kinetic stabilityPross has introduced the useful concept of dynamic kinetic
stability for describing the fate of systems in which replication
and selection occur concurrently [14]. The idea is that the
stability of a self-replicator in a system in which replication and
destruction processes occur simultaneously is not determined by
the thermodynamic stability of the replicator, nor by the rate of
formation of the replicator alone, but by the balance between
the rate of formation and the rate of destruction of the repli-
cator. As either replication or destruction (or both) are typically
coupled to other chemical reactions that convert high-energy
reactants to low-energy products, replication in a replication/
destruction regime should normally be chemically fueled. Such
fueling, in principle, allows complexification of the replicator,
without defying the second law of thermodynamics, as the
system as a whole still evolves towards increasing entropy.
With replicator complexification having been made feasible, it
then only depends on evolutionary possibilities and benefits
whether complexification also actually occurs.
In order for the considerations of dynamic kinetic stability to
apply and in order for Darwinian evolution to occur, it is essen-
tial that replicators are subjected to a replication–destruction
regime. Unfortunately, until now, very few systems reported in
the literature are (see below).
1.5 Open-ended evolutionAs mentioned before, the Darwinian triad of replication, selec-
tion, and mutation in itself is not sufficient to drive the
complexification of a chemical system. But what determines
whether a (chemical) system is capable of growing in complexi-
ty or is condemned to remain at a low level of complexity? This
is a question that is not only relevant in evolutionary chemistry,
but also has far-reaching consequences for the development of
artificial life in computer models. As Moreno and Ruiz-Mirazo
point out, in order for a system to fully evolve it should not only
exhibit structural variety, but also some form of functional
variety [17]. In the context of this review, we consider such
function as any property of the replicator that benefits the
dynamic kinetic stability of the system as a whole. A term that
is widely used to describe the emergence of novel functionality
is that of open-ended evolution. Although a clear consensus
about a definition of open-ended evolution is lacking in litera-
ture, we will adopt the definition provided by Taylor here.
Open-endedness means the capability of components in a
system to develop new forms continuously [18]. From this defin-
ition it follows that a self-replicating system should be able to
explore a huge number of possible mutants, otherwise the
system will either get trapped in a stationary optimum situation
or will recycle already explored forms of the replicator [19,20].
Both of these situations cannot lead to the continuous develop-
ment of new forms of replicators and are thus detrimental to the
open-endedness of the system. Another requirement is that the
total structural space available to the system should exceed by
many orders of magnitude the actual structural space that the
system occupies at any one time, or as Maynard-Smith and
Szathmáry put it; the replicators should possess unlimited
heredity [21]. It is also important to note that newly evolved
replicators are not necessarily more advanced or better than the
original replicator. It is the mere development of novelty that is
the vital aspect of open-ended evolution, causing it to be an
undirected process that does not necessarily entail progress
[18].
It is however not that trivial that a replicator can give rise to
such a large number of new forms. As Crutchfield and Schuster
pointed out, the dichotomy of genotype and phenotype is a
powerful mechanism to obtain such a vast number of possible
mutants [22]. Since mutations act on the genotype only and
selection pressure exclusively acts on the phenotype, the two
mechanisms are partially decoupled. If this were not the case
only those mutations that are favored by selection will occur,
strongly decreasing the possible number and randomness of
new forms of the replicator.
It is apparent that open-ended evolution plays an important role
in the emergence of novelty from simple replicators and that
Darwinian evolution alone is an insufficient requirement for
true unbounded evolution in a chemical system. This undirec-
tional evolutionary process is therefore considered to be of
importance in the transition from inanimate matter to life. The
exact principles governing open-ended evolution are however
not yet fully understood and it is not clear what the precise
requirements for a system are in order for it to be capable of
open-endedness [23].
In the following section we will discuss some basic principles
of self-replication, followed by a discussion on recent develop-
ments towards the realization of open-ended evolution in chem-
istry.
2 Replicating systemsThe most instructive and intuitive self-replicating system to
consider is probably that of DNA. A DNA molecule consists of
two strands of nucleotides that are intertwined to form a double
helix. During the replication process of DNA, each of these
strands can act as a template for the formation of a complemen-
tary strand. In this way an exact copy of the original structure of
DNA is formed and the DNA has successfully become repli-
cated. The replication of DNA however is a complex process
mediated by enzymes such as DNA polymerase and topoisom-
erase. To better understand the origin of life and as a possible
Beilstein J. Org. Chem. 2017, 13, 1189–1203.
1193
first step in the synthesis of de novo life it would be very inter-
esting indeed to achieve molecular replication without the need
of such enzymes, since enzymes themselves must be products
of an evolutionary process and can thus not explain the emer-
gence of living systems from basic chemical building blocks.
The following section will treat a representative selection of
self-replicating systems, for a more comprehensive overview,
see: Philp and Vidonne [24], Von Kiedrowski and Bag [25] and
Bissette and Fletcher [26].
2.1 Minimal self-replicating systemThe simplest form of a self-replicating system is that in which
the replicator acts as a catalyst for its own formation from a set
of basic building blocks. This fundamental form of a self-repli-
cating system is depicted in Figure 2 and is called a minimal
self-replicating system. An essential requirement for a minimal
replicating system is that molecules A and B are complementa-
ry to template T so that they are able to bind to it via noncova-
lent interactions.
Figure 2 shows three different channels in a minimal repli-
cating system. Building blocks A and B can react via the bimol-
ecular reaction pathway, to form the template molecule T. In
the second pathway – binary complex formation – A and B bind
together reversibly to form a complex [A∙B]. This complex may
undergo a covalent reaction if A and B experience an increased
effective molarity, leading to an inactive template Tinactive
which is folded back onto itself. The third pathway in the
minimal replication system is the autocatalytic cycle. In this
cycle, the building blocks A and B bind reversibly to the com-
plementary recognition sites on the template molecule T. This
arrangement brings molecules A and B in close proximity,
leading to an increased effective molarity and enhanced rate of
bond formation. When A and B ligate to each other, a [T∙T]
complex is formed, which can then dissociate to yield two iden-
tical T molecules. The autocatalytic cycle thus leads to a repli-
cation of the original template molecule. The final, and often
overlooked, pathway was identified by Reinhoudt et al.
following a fierce discussion between Rebek and Menger about
the mechanisms involved in the self-replication in their systems
[27]. In this pathway (not depicted in the diagram) one of the
building blocks, say A, binds to the template molecule. In
certain systems this can lead to the activation of A, such that B
can then react with A directly from solution.
Initially, when there are virtually no template molecules in the
mixture but only building blocks A and B, the bimolecular and
binary complex pathways leading to the formation of T and
Tinactive will be dominant. Clearly, the inactive template cannot
lead to autocatalysis and therefore hinders the self-replication
process. Upon formation of T, the autocatalytic pathway will
Figure 2: Minimal system for self-replication. Building blocks A and Bcan react to form either template T or its inactive counterpart Tinactive.The formation of template T can direct A and B to a configuration inwhich they are in close proximity, accelerating the reaction between Aand B leading to the formation of the [T∙T] complex. Dissociation of thiscomplex completes the replication cycle of the initial template mole-cule.
become increasingly important, in principle allowing for expo-
nential growth of the template. A requirement for effective
autocatalysis, however, is the dissociation of the [T∙T] complex
into two individual template molecules. If this complex does not
dissociate, the newly formed template molecule cannot lead to
further enhancement of the reaction rate, effectively arresting
the autocatalytic cycle. Such product inhibition is an important
limiting factor in many synthetic replicator systems and
prevents them from attaining exponential growth.
2.2 Reciprocal self-replicating systemA more complicated situation arises when the template mole-
cules under consideration are no longer self-complementary, but
instead are complimentary to a second template molecule. The
replication of DNA is a prime example of such a reciprocal self-
replicating system. One strand of the double helix acts as a tem-
plate for the formation of the other complementary strand and
vice versa. Figure 3 shows a schematic representation of a reci-
procal replicating system. It consists of two catalytic cycles
which both lead to the same template duplex [TCD∙TEF].
Instead of only two building blocks the reciprocal system has
four basic building blocks labeled C, D, E and F. Building
blocks C and D, can react to form the template TCD which
catalyzes the formation of the complementary template TEF
from building blocks E and F. Similarly the TEF template can
promote the formation of the TCD template.
Beilstein J. Org. Chem. 2017, 13, 1189–1203.
1194
Figure 3: A cross-catalytic replication scheme in which the formationof one template stimulates the formation of a different, complementarytemplate.
2.3 Reaction kinetics and its implicationsWhen considering a mixture containing only building blocks A
and B in the minimal replicator model (Figure 2), the formation
of template molecules T can initially only take place via the
bimolecular reaction pathway. The bimolecular reaction is a rel-
atively slow reaction, since it involves the unassisted formation
of a covalent bond between the two reactants. However, if a
sufficiently large amount of the template molecules is formed,
the autocatalytic cycle will play an increasingly dominant role.
Because the catalytic cycle leads to a doubling of the template
molecules after each run, an exponential increase in the concen-
tration of the reaction product would be expected. Naturally,
this exponential increase cannot continue indefinitely and will
slow down as the concentration of available building blocks
decreases. In summary, this would mean that for an idealized
minimal self-replicating system the concentration of the reac-
tion product T would show an S-like or sigmoidal shape.
A system in which product inhibition occurs, will not show
exponential growth (for exponential growth the kinetic order in
replicator r = 1) but only sub exponential growth. In many
cases r = 1/2 and the system is said to obey the square root law
of autocatalytic systems [28].
Figure 4: The first oligonucleotide capable of template directed self-replication without the need of enzymes. The depicted hexamer tem-plate T is formed from two trimer building blocks and catalyzes its ownformation. Self-reproduction of this molecule was shown to result inparabolic growth of the template concentration [30].
By seeding mixtures with different amounts of preformed tem-
plates T and measuring the initial rate of template formation, a
plot of log(d[T]/dt) versus log[T] can be constructed. From the
slope of this plot the reaction order r of the system can be deter-
mined [28]. It should however be considered that if the uncata-
lyzed bimolecular pathway (r = 0) also contributes to the for-
mation of T, the measured reaction order r reflects a weighted
average of the catalyzed and uncatalyzed pathways and can
therefore have a value smaller than 1, even for cases where the
autocatalytic pathway itself would have a reaction order r = 1.
In such situations computational simulations of the system can
provide additional information on the replication processes that
are involved [29].
2.4 Achieving exponential replicationPioneering work in the field of non-enzymatic self-replication
has been performed by the group of von Kiedrowksi, who was
the first to report on a template-directed self-replicating oligo-
nucleotide (Figure 4) [30]. To achieve template-directed self-
Beilstein J. Org. Chem. 2017, 13, 1189–1203.
1195
replication without the aid of enzymes, they used two trinu-
cleotides. Upon activation, these trinucleotides can condense to
form a hexamer template molecule T, depicted in Figure 4,
which catalyzes its own formation. The autocatalytic nature of
the reaction was proven by adding small amounts of preformed
template molecules to the reaction mixture. Kinetic analysis
revealed that the system exhibits parabolic replication (p = 1/2).
Exponential growth in this system is not obtained due to the
high thermodynamic stability of the [T∙T] dimer, leading to
product inhibition. Although the efficiency of the reported auto-
catalytic cycle is rather low, it still was a clear demonstration of
a template-directed self-replicating system and von Kiedrowski
did not fail to recognize the potential of natural selection in
such systems.
Later research focused on overcoming the product inhibition
problem in order to obtain exponential instead of parabolic
growth of the replicators. A successful approach to overcoming
product inhibition involves the immobilization of the template
molecules by fixing them onto a solid support. This approach
was partially inspired by the notion that surfaces of minerals
might have played a major role in catalyzing the formation of
biopolymers [31,32]. Von Kiedrowski et al. were able to
demonstrate exponential growth of oligonucleotides using a
method that they gave the eloquent anagram; SPREAD (Sur-
face-Promoted Replication and Exponential Amplification of
DNA analogues) [33]. In the SPREAD technique, depicted in
Figure 5, an oligonucleotide template strand is immobilized via
an irreversible interaction with a solid support. A complementa-
ry strand is then produced via the template-directed binding of
free nucleotides from the solution. The copied strand is re-
leased from the template and is in turn itself immobilized on a
solid support, thereby preventing product inhibition via the for-
mation of stable template dimers. As von Kiedrowski and
coworkers rightfully notice, this system allows for evolutionary
processes to take place. Moreover, such immobilized systems
are proposed to be even capable of amplification of mutations.
The introduction of mutations can lead to a weaker base pairing
between the template molecule and its copy, thus increasing the
efficiency of the separation of this particular template duplex.
Considering the proposed abundance of amino acids, it is
natural to assume the presence of peptides and oligopeptides
under prebiotic conditions. However, initially only very short
peptides were produced in experiments under such conditions,
raising doubts over their potential role as a precursor of life.
When forming α-helices however, longer polypeptides can be
stabilized by the formation of coiled-coil motifs as in Figure 6.
If every a and d position of each individual helix is occupied by
a hydrophobic amino acid, the helices can intertwine and bury
their hydrophobic side groups into each other. This hydro-
Figure 5: Replication involving the SPREAD technique which preventsproduct inhibition. (1) A template molecule is immobilized on a solidsupport and (2, 3) a complementary copy is produced by template-directed replication. Finally the copied strand is (4) released from thetemplate and is in turn immobilized [33].
Figure 6: Figure showing (a) a coiled coil motif due to hydrophobicinteractions between hydrophobic amino acids in the individual helices.(b) Helical-wheel diagram showing how the hydrophobic amino acidssituated on the a and d sites can interact with each other to form thecoiled coil [34].
phobic interaction that drives the formation of coiled-coil motifs
can be further enhanced by electrostatic interactions between
amino acids residing on the c and g positions of the α-helices.
Ghadiri et al. showed that such coiled-coil peptides are capable
of self-replication [35]. As depicted in Figure 7, helical
polypeptides can act as a template for shorter peptide fragments
by means of molecular recognition. The peptide building blocks
again are ligated, resulting in the formation of a template duplex
with a coiled-coil motif. When separated from the original tem-
plate, a copy of the template is obtained. Initially these repli-
Beilstein J. Org. Chem. 2017, 13, 1189–1203.
1196
Figure 7: Self-replication of a helical peptide. Molecular recognitionleads to the formation of a stable coiled coil structure from smallerpeptide fragments. Depending on the length and stability of the coiledcoil structure, the template-duplex dissociates in the original templateand a copy [37].
cating systems were reported to show only parabolic growth,
because of the very high stability of the coiled-coil structure.
This problem was later addressed by Issac and coworkers by
reducing the length of the template molecule, which led to a de-
creased stability of the template duplex. Using this approach
they obtained near exponential growth of the template concen-
tration of p = 0,91 [36,37]. The above examples all illustrate
that, while not trivial, it is indeed possible to obtain self-repli-
cating behavior in the absence of enzymes. While this marks a
significant contribution to our understanding of the early stages
of the transition from chemistry to biology, it does not directly
explain the emergence of the RNA and DNA dominated world
as we know it, which would probably have required open-ended
evolution.
3 Evolutionary dynamics of replicators3.1 Enzyme mediated replicationIconic early experiments aiming to achieve Darwinian type
evolution in a chemical system were performed by Spiegelman
et al. in 1967 [3]. RNA replicase and a small input of genomic
RNA were successfully isolated from the bacteriophage Qβ.
The RNA molecules in this system are replicated by an RNA
replicase enzyme. By successive rounds of amplification and
selection, selection pressure was introduced to the system by
favoring fast reproducing entities of the genomic RNA. Since
shorter sequences are being replicated at a higher rate than
longer sequences, shortened mutants are favored over longer se-
quences. This eventually led to a strong decrease in the genome
size of the RNA molecules. However, this result is not as trivial
as it may seem at first sight, since it is of vital importance that
the mutant species do not lose their ability to be replicated, indi-
cating that only specific parts of the genome that are not needed
for recognition by the polymerase were deleted. Although the
RNA molecules involved are not self-replicating but are repli-
cated by the RNA replicase, the study still marks a starting
point in the field of in vitro evolution. Later, Braun et al.
managed to apply a selection pressure that favors the replica-
tion of long DNA sequences over short strands by creating heat
gradients in pores that act as a thermal trap [38]. The thermal
traps selectively retain longer DNA sequences, thereby effec-
tively overcoming the inherent advantage of the replication of
short sequences.
3.2 Dynamics of self-replicatorsAshkenasy recently reported a peptide based synthetic autocat-
alytic network that shows two significantly distinct steady states
depending on the history of the system [39]. Depending on the
initial concentration of replicator molecules provided to the
system, the system will reach either a low or a high steady state
replicator concentration. Switching between these two states
can be achieved by applying external stimuli in the form of heat
or the addition of decomposing agents. The switchable behav-
ior and memory of such a self-replicating system constitute an
exciting step, moving systems of self-replicating molecules
away from equilibrium, with potential impact on evolutionary
behavior [40].
Another interesting dynamic emergent property of self-repli-
cating systems was demonstrated by Philp and coworkers [41].
They showed how self-replicating molecules can create a reac-
tion-diffusion front when seeded to a homogeneous mixture of
building blocks. Dynamically evolving out-of-equilibrium envi-
ronments like these could enable interesting behavior of replica-
tors that is not achievable in homogenous reaction mixtures. It
will be very exciting to observe the evolutionary behavior of
mixtures of replicators in such spatially resolved environments.
3.3 RNA self-replicationOwing to the importance of RNA in viral species and in the
origin of life, evolution experiments are most often performed
using RNA molecules or closely related derivatives. In fact, it
has become possible to perform natural selection on oligo-
nucleotides by iterative amplification and selection processes
using a technique called systematic evolution of ligands by
exponential enrichment, or SELEX. In SELEX, a library of
DNA and RNA sequences is exposed to a certain target. In
multiple selection rounds the binding species are selected and
amplified, while the non-binding DNA and RNA molecules are
disposed of. In this way molecules are evolved based on their
ability to bind to a specific target [42,43].
However, these in vitro evolution experiments all exploit RNA-
based enzymes (ribozymes) or proteins in their replication
process to obtain exponential growth and are consequently not
self-replicating. Efforts have been made to obtain in vitro evolu-
tion of RNA in the absence of any enzymes. Unfortunately, the
demonstration of multiple cycles of non-enzymatic RNA repli-
Beilstein J. Org. Chem. 2017, 13, 1189–1203.
1197
Figure 8: (a) Cross-catalyzed replication of template molecules E and E’ from their building blocks A(’) and B(’). (b) Secondary structure of the tem-plate duplex. The curved arrow denotes the site of ligation of the building blocks, the dashed boxes include the sequences to be mutated and the solidlines indicate the sites of the G∙U base pairs inducing the wobble that enhances catalytic activity. (c) The altered sequences of the 12 different tem-plate molecules, the E’ molecules have complementary sequences in the base pairing part (horizontal) and identical sequences in the catalytic part(vertical). Dark circles denote the differences relative to E1 [45].
cation in a test tube is troubled by the fact that the RNA duplex
that is formed upon replication is quite stable and can have
dissociation temperatures as high as 90 °C [44]. Without an en-
zyme that separates the newly created strands, this stability
would lead to product inhibition, halting the self-replication
process.
3.4 Cross-catalyzing RNA replicatorsJoyce and Lincoln showed, however, that a system of two RNA
enzymes can catalyze each other’s synthesis from a mixture of
four different building blocks via template-directed reciprocal
replication [45]. The RNA ligase molecule E can bind two
oligonucleotide building blocks A’ and B’ and promote their
ligation to form the ligase E’. The newly formed ligase E’ can
then in turn promote the formation of E, as depicted in
Figure 8a. But this cross-catalytic reaction typically occurs at a
very slow rate. In order to enhance this rate, enzymatic in vitro
evolution of the RNA molecules was performed in order to
obtain a set of fast replicating species.
It was found from in vitro evolution experiments that the intro-
duction of G∙U base pairs close to the site of ligation leads to
enhanced cross-catalytic activity. Figure 8b shows the se-
quence and secondary structure of the A∙B∙E’ complex. The site
of ligation is indicated by the curved arrow and the G∙U pairs
that are depicted in a solid box induce a wobble in the sequence
that results in the enhanced catalytic activity. When this wobble
is installed in both enzymes of the cross-catalytic set, exponen-
Beilstein J. Org. Chem. 2017, 13, 1189–1203.
1198
tial growth of the system can be achieved over multiple cycles.
With an exponential replicator in hand, Darwinian evolution in
a cross-catalytic system lies within reach. To study this, Joyce
and his team prepared 12 pairs of cross-catalytic enzymes and
their corresponding building blocks, that have alteration in parts
of the sequence denoted by the dashed line in Figure 8b. The
different pairs are denoted as E1 to E12 and are shown in
Figure 8c. It is important to note that mutations between en-
zymes are such that the stability of the ligase duplex due to base
pairing is not altered, but only the catalytic activity and replica-
tion rate are affected. All these enzymes were shown to cross-
replicate, with the E1 pair showing the highest rate of replica-
tion.
A serial transfer experiment was performed on a mixture that
contained the 12 different enzyme pairs and their correspond-
ing 48 building blocks (A1, A1’, B1, and B1’ for pair E1, for
example). In such a serial transfer experiment a small percent-
age, in this case 5%, is transferred to a new reaction mixture
after a replication round took place. This effectively eliminates
the slow replicators that are only present in small quantities in
the mixture so that they tend to go extinct. The transferred repli-
cators, however, are presented with a fresh batch of building
blocks and can continue to replicate. By doing this for multiple
rounds, large amplification factors can be achieved. For this ex-
periment it is important to realize that A1 does not necessarily
have to be ligated to B1, but that it can ligate to any of the other
B-type building blocks, although they may be mismatched to
the template. This freedom of recombination leads to 132
possible combinations of building blocks. After 20 successive
transfers a 1025-fold amplification was reached. A sample of
100 of these clones contained only 7 non-recombinant clones,
whereas the rest were all ligated to building blocks that were
not their original partners. Figure 9 shows the distribution of
different E (dark columns) and E’ (light columns) enzymes in
the final sample. This result shows how fitter replicators can
come to dominate the population after several rounds of ampli-
fication. Fitness of the molecules depends in this case on their
ability to perform cross-catalytic replication with other mole-
cules.
This study by Joyce et al. demonstrates how selection pressure
can lead to certain replicators dominating a population in a
cross-catalytic replication process. However, the environmental
conditions in this experiment are static and the system lacks
open-endedness because the number of building blocks that is
provided to the system restricts the total diversity of the
newly formed species, in this case 12 × 12 different possible
replicators. This will cause the system to reach a steady state in
which no novel forms of the replicator can be explored
anymore.
Figure 9: Distribution of the species present in the reaction mixtureafter 20 serial transfers. E and E’ molecules are represented by thedark and light shaded bars, respectively. Note how certain specieshave come to dominate the population, particularly A5B3. Moreover,only 7 molecules were found to be paired to their original partner (cor-responding to the shaded diagonal) [45].
3.5 Cooperative catalytic systemThe concept of such a cross-replicating system can be readily
extended to higher order systems, involving three, four or even
more components. Eventually, one could envision an entire
network of cross-replicating molecules. Lehman et al. showed
that a mixture of relatively short RNA segments can self-
assemble to form self-replicating ribozymes [46]. These
ribozymes in turn gave rise to spontaneous formation of cooper-
ative networks that were shown to grow faster than the autocat-
alytic replication rate of the individual ribozymes. Moreover,
cooperative systems are generally more stable towards para-
sites then autocatalytic self-replicators and are, in principle, able
to gain in complexity [46,47].
In the study a ribozyme of around 200 nucleotides called
Azoarcus was used. This ribozyme is made from four different
RNA strands (W, X, Y and Z) that can self-assemble cova-
lently in an autocatalytic manner, as depicted in Figure 10a. The
effectiveness of this self-replication process depends on the
ability of the internal guide strand (IGS) to recognize its target.
To form a cooperative set, the Azoarcus ribozyme was frag-
mented in two different pieces in three different ways, creating
three different pairs I1, I2 and I3 which are shown encircled in
Figure 10b. Furthermore, the target and IGS sequences were
altered such that autocatalytic self-replication is minimized. The
sequence was, however, chosen such that the IGS of one pair is
matched to the target sites of the next pair. In this way one
ribozyme, say E1, can catalyze the formation of the next
Beilstein J. Org. Chem. 2017, 13, 1189–1203.
1199
Figure 10: (a) Secondary structure of the Azoarcus ribozyme consisting of four different strands of RNA, W, X, Y, and Z. Self-replication is mediatedby recognition of the target sites by the IGS (grey boxes), leading to ligation of the strands. The dashed line indicates the catalytic core of the result-ing ribozyme. (b) Cooperative replicating system. The formation of the covalent ribozyme E3 from the non-covalent I3 complex is catalyzed by E2ribozyme. The formation of this E2 is in turn catalyzed by E1, which is catalyzed by E3, resulting in a cyclic dependence. Numbers above the arrowsdenote the advantage of cooperativity [46].
ribozyme, E2, from its non-covalently bound building blocks
I2. This ribozyme can in turn catalyze the formation of E3 from
its building block and finally, to close the cycle, E3 can cata-
lyze the formation of the E1 ribozyme. This cooperative system
is depicted in Figure 10b and it was observed that a mixture
containing all three pairs resulted in a much higher yield of full-
length RNA (a factor 125) than obtained from the sum of the
isolated pairs, proving that the system replicates in a coopera-
tive manner.
Interestingly, it was shown that in isolation the autocatalytic
replicators (with the IGS programmed to recognize itself) repli-
cated faster than the cross-catalytic system, whereas in a mix-
ture of all different components the cooperative network grows
faster than the selfishly replicating molecules. However, this
result was obtained using deliberately designed pairs with spe-
cific targets. Behavior becomes a lot more fascinating when one
of the nucleotides of the IGS (M) and target sites (N) is random-
ized, creating a mixture of 48 matched and unmatched pairs in
total, as schematically depicted in Figure 11a. After incubation
of all six sets of Figure 11a for several hours, all of these 48
possible sequences were indeed found in the mixture. Initially
the replication is dominated by autocatalytic cycles in which N
and M are complimentary. This initial rise of the autocatalytic
replicators is depicted in Figure 11b by the dashed line with
crosses, the contribution of the two-membered cycles is
depicted by the dashed lines with dots (depicted value ×10). At
later times a transition to the more complex three-membered
cycles was observed as witnessed by the rise of the solid line
(×10.000). After 8 hours, it was observed that replication occurs
increasingly via cooperative cycles and that all genotypes con-
tribute increasingly with time. This result shows how an
initially autocatalytic cycle can give rise to increasingly com-
plex systems of cooperative replication over time. Interestingly,
the overall replication efficiency of the randomized multi-com-
ponent network exceeded that of the engineered 3-component
network in Figure 10b.
To better mimic prebiotic conditions in which iterations over
multiple generations would have occurred, a serial transfer ex-
periment using the same set of replicators was also performed.
In this experiment an aliquot of the reaction mixture is trans-
ferred to a new flask with building blocks every hour, so that
the more stable and fast replicating molecules and networks are
favored. Again a transition from autocatalytic cycles to more
complex systems was observed.
Beilstein J. Org. Chem. 2017, 13, 1189–1203.
1200
Figure 11: (a) The different combinations of IGS strands, tags andbreak junction give rise to a total of 48 different pairs. (b) Graphshowing the frequency of autocatalytic replicators (dashed, crosses),the two-membered cycles (dashed, dots; ×10) and the three-mem-bered cycles (solid; ×10.000) over time. Note the emergence of themore complex three-membered cycles at later times [46].
Such cooperative systems are capable of complexification and
natural selection and can therefore be of importance in bridging
the gap between replication of simple short RNA molecules
from nucleotide building blocks and the formation of more
complex ribozymes. The observed cooperative behavior relies
on recognition strands and tags, so that it will only play a role
for the assembly of intermediate-sized oligonucleotides. Small
oligonucleotides would likely still replicate more efficiently via
auto or cross catalytic cycles. At a certain length scale the for-
mation of cooperative systems becomes favorable and these
mechanisms might take over the replication process, allowing
for complexification and diversification of the system. Howev-
er, since the replication of each member is dependent on one or
more other members of the system, the members should all be
in close proximity to each other in order to obtain a stable
system. This requires high concentrations of the reaction mix-
ture, which is of course readily achieved in the laboratory but is
probably less likely under prebiotic conditions. In order to
increase the concentration of replicators locally, a specialized
compartmentalization should act in concert with the coopera-
tive replication system. How such compartmentalization might
occur is another topic entirely and beyond the scope of this
review, but it is proposed that compartmentalization can actu-
ally aid in the evolution of replicating molecules [48-50].
3.6 Diversification of self-replicatorsOther types of molecules than RNA that are capable of self-
replication and information storage are showing interesting
results in the study of open-ended evolution and the synthesis of
life as well [51]. Recently, we have demonstrated a self-repli-
cating system involving peptides capable of diversification
using a systems chemistry approach [52]. Following the
discovery of an exponentially growing self-replicating system
[53], we used two building blocks, 1 and 2, to form a dynamic
combinational library (DCL) of self-replicating molecules.
These building blocks consist of an aromatic core that is func-
tionalized with two thiol groups and a peptide chain
(Figure 12a). Building block 1 and 2 are very closely related to
each other and differ only in a single amino acid of the peptide
chain. These peptide building blocks can then be oxidized to
form macrocycles of different sizes as depicted in Figure 12b.
The design of the peptide chains is such that self-assembly of
the chains into parallel β-sheets is promoted, which in turn leads
to the formation of stacks of macrocycles as shown in
Figure 12c. Growth of these stacks occurs exclusively via the
ends of the fibers and it is therefore not surprising that the reac-
tion rate is strongly dependent on the amount of fibers present
in the mixture. As soon as a fiber reaches a critical length it can
fragment when mechanically agitated. When fragmentation
occurs, the number of available fiber ends is doubled, leading to
an exponential self-replication.
In previous work it was already shown that the less hydro-
phobic building block 2 tends to form larger octameric macro-
cycles than the more hydrophobic building block 1 which forms
hexamers [54]. This is reasonable, since a weaker hydrophobic
interaction provided by 2 would need more individual interac-
tions in order to achieve the same stability as a more hydro-
phobic counterpart 1.
By using a mixture containing two different building blocks
instead of one, the replicators can potentially undergo mutation
by incorporating a different building block into their structures.
A mixture with equal concentrations of both building blocks
was prepared and monitored over the course of 35 days.
Initially a complex mixture of four different trimers and five
different tetramers was observed. After some days, however, a
set of hexamers which was enriched in building block 1 arose in
the mixture (set I) as shown by the red line in Figure 13. As the
emergence of set I depletes the mixture from building block 1
the environmental conditions are essentially changed up to the
point where a second set of hexamers arises which is rich in
building block 2.
It was shown that set I is the ancestor of set II. When macro-
cycles that are rich in building block 2 are exposed at the fiber
Beilstein J. Org. Chem. 2017, 13, 1189–1203.
1201
Figure 12: Figure depicting (a) building blocks consisting of a peptide attached to an aromatic ring. Building blocks 1 and 2 differ only in the nature ofthe penultimate amino acid. (b) The building blocks can form macrocycles of different sizes upon oxidation, which can exchange building blocks witheach other. (c) Schematic representation showing how building blocks oxidize to form macrocycles that in turn form stacks due to β-sheet formation.Stacks grow from their ends and fragment upon agitation, leading to more fiber ends and faster growth [52].
ends of set I, they act as a template for the formation of
members of set II. Indeed, significant amounts of set II
members only form when a seed of set I is present that contains
2-enriched members. Set I is therefore able to transfer informa-
tion about its macrocyclic size to set II. This process bears a
crude resemblance to how species originate in biology.
ConclusionSelf-replicating molecules have been remarkably hard to
develop and after 30 years of research there are still only a
handful of efficient self-replicators. Achieving Darwinian
evolution with these systems has proven even more challenging.
The evolutionary potential of many self-replicating molecules is
limited due to the fact that it is difficult to achieve exponential
growth of the replicator. Factors limiting the efficiency of the
self-replication process are the presence of non-autocatalytic
pathways and product inhibition. Methods aiming to minimize
the effect of product inhibition, like the SPREAD technique and
the destabilization of template-duplexes, have successfully been
developed to allow for exponential growth of some simple
Beilstein J. Org. Chem. 2017, 13, 1189–1203.
1202
Figure 13: Plot showing the relative concentrations of set I (red), set II(blue) and the link between them; (1)3(2)3 (purple). Note how at firstonly set I is present in the mixture, while at some point this set givesrise to the descendant set II. [52]
replicators. Also mechanical forces may be utilized to break up
larger assemblies of self-replicating molecules and liberate the
assembly edges or fiber ends that promote replication.
The most impressive progress with respect to Darwinian evolu-
tion has been achieved with RNA-based cross-replicators. In
serial transfer experiments changes in replicator populations
were observed that were not immediately predictable and that
favored the most efficient replicators or networks of cooper-
ating replicators. What these systems have not (yet) shown is
the emergence of new functions that contribute to the dynamic
kinetic stability of the replicators.
The true challenge of any in vitro evolution experiment lies in
the realization of a system that has the capability to undergo
open-ended evolution. Such systems can diversify and increase
in complexity and invent new functions indefinitely. Until now,
chemical systems that show evolutionary behavior have
involved relatively simple replicators that only had access to a
very limited structural space of possible mutations. This rapidly
causes the system to be incapable of exploring new structures
and the development of novelty will stagnate. An additional
limitation of simple replicators is the strong relation between
their genotype and phenotype. This lack of dichotomy causes
the mechanisms of mutation and natural selection to couple to
each another, hampering the evolvability of the systems. It is far
from trivial to design a system that is simple enough to be
capable of exponential replication and has a large structural
space of mutations at the same time. Yet a push in this direc-
tion is probably needed, expanding the structural space avail-
able for existing replicators to explore, enabling them to
discover new functions, one of which might eventually be the
decoupling between genotype and phenotype, which would
allow the system to explore a dramatically larger structural and
functional space.
Besides these issues concerning the design of replicators, it is
still not studied in detail how the environment of the replicators
can interact with the evolutionary process. Can environmental
conditions like acidity or temperature, for instance, be an incen-
tive towards the development of novel functionalities in the
replicators? And how is the notion of death introduced in an ex-
periment in which the researcher does not actively intervene
with the system through, for example, serial dilution? In any
true open-ended system replicators interact with the environ-
ment on their own account and are not steered by the experi-
menter to a significant extent.
Thus, the challenge is now to design systems of self- or cross-
replicating molecules that can access and evolve into a vast
structural and functional space and facilitate, by appropriate
design of building blocks and experimental conditions, the
invention of new functions and thereby achieve open-ended
evolution.
AcknowledgementsH. D. is grateful for the scholarship granted by the Zernike
Institute for Advanced Materials. We also acknowledge the
ERC, the NWO and the Dutch Ministry of Education, Culture
and Science (Gravitation Program 024.001.035) and COST
CM1304.
References1. Kauffmann, S. A. At Home in the Universe; Oxford University Press:
New York, USA, 1995.2. Darwin, C. On the Origin of Species; D. Appleton and CO.: New York,
USA, 1871.3. Mills, D. R.; Peterson, R. L.; Spiegelman, S.
Proc. Natl. Acad. Sci. U. S. A. 1967, 58, 217–224.doi:10.1073/pnas.58.1.217
4. Joyce, G. F. Angew. Chem., Int. Ed. 2007, 46, 6420–6436.doi:10.1002/anie.200701369
5. Szathmary, E.; Gladkih, I. J. Theor. Biol. 1989, 138, 55–58.doi:10.1016/S0022-5193(89)80177-8
6. Lifson, S.; Lifson, H. J. Theor. Biol. 2001, 212, 107–109.doi:10.1006/jtbi.2001.2361
7. Joyce, G. F. Annu. Rev. Biochem. 2004, 73, 791–836.doi:10.1146/annurev.biochem.73.011303.073717
8. Eigen, M.; McCaskill, J.; Schuster, P. J. Phys. Chem. 1988, 92,6881–6891. doi:10.1021/j100335a010
9. Ruiz-Mirazo, K.; Briones, C.; De la Escosura, A. Chem. Rev. 2014,114, 285–366. doi:10.1021/cr2004844
10. Eigen, M. Proc. Natl. Acad. Sci. U. S. A. 2002, 99, 13374–13376.doi:10.1073/pnas.212514799
11. Arenas, C. D.; Lehman, N. BMC Evol. Biol. 2010, 10, 80.doi:10.1186/1471-2148-10-80
Beilstein J. Org. Chem. 2017, 13, 1189–1203.
1203
12. Biebricher, C. K.; Eigen, M. Virus Res. 2005, 107, 117–127.doi:10.1016/j.virusres.2004.11.002
13. Crotty, S.; Cameron, C. E.; Andino, R. Proc. Natl. Acad. Sci. U. S. A.2001, 98, 6895–6900. doi:10.1073/pnas.111085598
14. Pascal, R.; Pross, A. Synlett 2017, 30–35.doi:10.1055/s-0036-1589403
15. Ruiz-Mirazo, K.; Pereto, J.; Moreno, A. Origins Life Evol. Biospheres2004, 34, 323–346. doi:10.1023/B:ORIG.0000016440.53346.dc
16. Taylor, T. European conference on artificial life 2015, York, UK, July,2015.
17. Moreno, A.; Ruiz-Mirazo, K. Biol. Philos. 2009, 24, 585–605.doi:10.1007/s10539-009-9178-6
18. Taylor, T. J. From Artificial Evolution to Artificial Life. Ph.D. Thesis,University of Edinburgh, U.K., 1999.
19. Von Neumann, J.; Burks, A. W. IEEE Trans. Neural Networks 1966, 5,3–14.
20. Ruiz-Mirazo, K.; Umerez, J.; Moreno, A. Biol. Philos. 2008, 23, 67–85.doi:10.1007/s10539-007-9076-8
21. Szathmáry, E.; Maynard Smith, J. Nature 1995, 374, 227–232.doi:10.1038/374227a0
22. Crutchfield J.P.; Schuster, P. Genotype and phenotype. In EvolutionaryDynamics: Exploring the Interplay of Selection, Accident, Neutrality,and Function, Oxford University Press: Oxford, U.K., 2003; pp 164-169.
23. Taylor, T.; Bedau, M.; Channon, A.; Ackley, D.; Banzhaf, W.;Beslon, G.; Dolson, E.; Froes, T.; Hickinbotham, S.; Ikegami, T.;McMullin, B.; Packard, N.; Rasmussen, S.; Virgo, N.; Agmon, E.;Clarck, E.; McGregor, S.; Ofria, C.; Ropella, G.; Spector, L.;O. Stanley, K.; Stanton, A.; Timperley, C.; Vostinar, A.; Wiser, M.Artif. Life 2016, 22, 408–423. doi:10.1162/ARTL_a_00210
24. Vidonne, A.; Philp, D. Eur. J. Org. Chem. 2009, 5, 593–610.doi:10.1002/ejoc.200800827
25. Bag, B. J.; Von Kiedrowski, G. Pure Appl. Chem. 2009, 68, 2145–2152.doi:10.1351/pac199668112145
26. Bissette, A. J.; Fletcher, S. L. Angew. Chem., Int. Ed. 2013, 52,12800–12826. doi:10.1002/anie.201303822
27. Reinhoudt, D. N.; Rudkevich, D. M.; De Jong, F. J. Am. Chem. Soc.1996, 118, 6880–6889. doi:10.1021/ja960324g
28. Von Kiedrowski, G. Bioorg. Chem. Front. 1993, 3, 113–146.29. Coulomb-Delsuc, M.; Mattia, E.; Sadownik, J. W.; Otto, S.
Nat. Commun. 2015, 6, 7427. doi:10.1038/ncomms842730. Von Kiedrowski, G. Angew. Chem., Int. Ed. Engl. 1986, 25, 932–935.
doi:10.1002/anie.19860932231. Ferris, J. P.; Hill, A. R.; Liu, R.; Orgel, L. E. Nature 1996, 381, 59–61.
doi:10.1038/381059a032. Ferris, J. P.; Ertem, G. Science 1992, 257, 1387–1389.
doi:10.1126/science.152933833. Luther, A.; Brandsch, R.; Von Kiedrowski, G. Nature 1998, 396,
245–248. doi:10.1038/2434334. Armstrong, C. T.; Boyle, A. L.; Bromley, E. H. C.; Mahmoud, Z. N.;
Smith, L.; Thomson, A. R.; Woolfson, D. N. Faraday Discuss. 2009,143, 359–372. doi:10.1039/B915411F
35. Lee, D. H.; Granja, J. R.; Martinez, J. A.; Severin, K.; Ghadiri, M. R.Nature 1996, 382, 525–528. doi:10.1038/382525a0
36. Issac, R.; Chmielewski, J. J. Am. Chem. Soc. 2002, 124, 6808–6809.doi:10.1021/ja026024i
37. Issac, R.; Ham, Y. W.; Chmielewski, J. Curr. Opin. Struct. Biol. 2001,11, 458–463. doi:10.1016/S0959-440X(00)00233-5
38. Kreysing, M.; Keil, L.; Lanzmich, S.; Braun, D. Nat. Chem. 2015, 7,203–208. doi:10.1038/nchem.2155
39. Mukherjee, R.; Cohen-Luria, R.; Wagner, N.; Ashkenasy, G.Angew. Chem., Int. Ed. 2015, 54, 12452–12456.doi:10.1002/anie.201503898
40. Decker, P. Nature (London) 1973, 241, 72–74.doi:10.1038/newbio241072a0
41. Bottero, I.; Huck, J.; Kosikova, T.; Philp, D. J. Am. Chem. Soc. 2016,138, 6723–6726. doi:10.1021/jacs.6b03372
42. Keefe, A. D.; Pai, S.; Ellington, A. Nat. Rev. Drug Discovery 2010, 9,537–550. doi:10.1038/nrd3141
43. Mahlknecht, G.; Maron, R.; Mancini, M.; Schechter, B.; Sela, M.;Yarden, Y. Proc. Natl. Acad. Sci. U. S. A. 2013, 110, 8170–8175.doi:10.1073/pnas.1302594110
44. Hernandez, A. R.; Piccirilli, J. A. Nat. Chem. 2013, 5, 360–362.doi:10.1038/nchem.1636
45. Lincoln, T. A.; Joyce, G. F. Science 2009, 323, 1229–1232.doi:10.1126/science.1167856
46. Vaidya, N.; Manapat, M. L.; Chen, I. A.; Xulvi-Brunet, R.; Hayden, E. J.;Lehman, N. Nature 2012, 491, 72–77. doi:10.1038/nature11549
47. Higgs, P. G.; Lehman, N. Nat. Rev. Genet. 2015, 16, 7–17.doi:10.1038/nrg3841
48. Ghadessy, F. J.; Ong, J. L.; Holliger, P. Proc. Natl. Acad. Sci. U. S. A.2001, 98, 4552–4557. doi:10.1073/pnas.071052198
49. Szostak, J. W.; Bartel, D. P.; Luisi, P. L. Nature 2001, 409, 387–390.doi:10.1038/35053176
50. Matsumura, S.; Kun, A.; Ryckelynck, M.; Coldren, F.; Szilágyi, A.;Jossinet, F.; Rick, C.; Nghe, P.; Szathmáry, E.; Griffiths, A. D. Science2016, 354, 1293–1296. doi:10.1126/science.aag1582
51. Pinheiro, V. B.; Taylor, A. I.; Cozens, C.; Abramov, M.; Renders, M.;Zhang, S.; Chaput, J. C.; Wengel, J.; Peak-Chew, S. Y.;McLaughlin, S. H.; Herdewijn, P.; Holliger, P. Science 2012, 336,341–344. doi:10.1126/science.1217622
52. Sadownik, J. W.; Mattia, E.; Nowak, P.; Otto, S. Nat. Chem. 2016, 8,264–269. doi:10.1038/nchem.2419
53. Carnall, J. M. A.; Waudby, C. A.; Belenguer, A. M.; Stuart, M. C. A.;Peyralans, J. J. P.; Otto, S. Science 2010, 327, 1502–1506.doi:10.1126/science.1182767
54. Malakoutikhah, M.; Peyralans, J. J. P.; Colomb-Delsuc, M.;Fanlo-Virgós, H.; Stuart, M. C. A.; Otto, S. J. Am. Chem. Soc. 2013,135, 18406–18417. doi:10.1021/ja4067805
License and TermsThis is an Open Access article under the terms of the
Creative Commons Attribution License
(http://creativecommons.org/licenses/by/4.0), which
permits unrestricted use, distribution, and reproduction in
any medium, provided the original work is properly cited.
The license is subject to the Beilstein Journal of Organic
Chemistry terms and conditions:
(http://www.beilstein-journals.org/bjoc)
The definitive version of this article is the electronic one
which can be found at:
doi:10.3762/bjoc.13.118